US20200343090A1 - Method for manufacturing semiconductor film - Google Patents
Method for manufacturing semiconductor film Download PDFInfo
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- US20200343090A1 US20200343090A1 US16/805,767 US202016805767A US2020343090A1 US 20200343090 A1 US20200343090 A1 US 20200343090A1 US 202016805767 A US202016805767 A US 202016805767A US 2020343090 A1 US2020343090 A1 US 2020343090A1
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- 239000004065 semiconductor Substances 0.000 title claims abstract description 181
- 238000000034 method Methods 0.000 title claims abstract description 64
- 238000004519 manufacturing process Methods 0.000 title claims abstract description 52
- 230000001678 irradiating effect Effects 0.000 claims abstract description 12
- JNDMLEXHDPKVFC-UHFFFAOYSA-N aluminum;oxygen(2-);yttrium(3+) Chemical group [O-2].[O-2].[O-2].[Al+3].[Y+3] JNDMLEXHDPKVFC-UHFFFAOYSA-N 0.000 claims description 5
- 229910019901 yttrium aluminum garnet Inorganic materials 0.000 claims description 5
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims description 4
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Images
Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02518—Deposited layers
- H01L21/02521—Materials
- H01L21/02524—Group 14 semiconducting materials
- H01L21/02532—Silicon, silicon germanium, germanium
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02656—Special treatments
- H01L21/02664—Aftertreatments
- H01L21/02667—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth
- H01L21/02675—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth using laser beams
- H01L21/02686—Pulsed laser beam
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02656—Special treatments
- H01L21/02664—Aftertreatments
- H01L21/02667—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth
- H01L21/02691—Scanning of a beam
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/66007—Multistep manufacturing processes
- H01L29/66075—Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials
- H01L29/66227—Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials the devices being controllable only by the electric current supplied or the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched, e.g. three-terminal devices
- H01L29/66409—Unipolar field-effect transistors
- H01L29/66477—Unipolar field-effect transistors with an insulated gate, i.e. MISFET
- H01L29/66742—Thin film unipolar transistors
- H01L29/6675—Amorphous silicon or polysilicon transistors
- H01L29/66765—Lateral single gate single channel transistors with inverted structure, i.e. the channel layer is formed after the gate
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02436—Intermediate layers between substrates and deposited layers
- H01L21/02439—Materials
- H01L21/02488—Insulating materials
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02518—Deposited layers
- H01L21/02587—Structure
- H01L21/0259—Microstructure
- H01L21/02592—Microstructure amorphous
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L27/00—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate
- H01L27/02—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers
- H01L27/12—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers the substrate being other than a semiconductor body, e.g. an insulating body
- H01L27/1214—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers the substrate being other than a semiconductor body, e.g. an insulating body comprising a plurality of TFTs formed on a non-semiconducting substrate, e.g. driving circuits for AMLCDs
- H01L27/1259—Multistep manufacturing methods
- H01L27/127—Multistep manufacturing methods with a particular formation, treatment or patterning of the active layer specially adapted to the circuit arrangement
- H01L27/1274—Multistep manufacturing methods with a particular formation, treatment or patterning of the active layer specially adapted to the circuit arrangement using crystallisation of amorphous semiconductor or recrystallisation of crystalline semiconductor
- H01L27/1285—Multistep manufacturing methods with a particular formation, treatment or patterning of the active layer specially adapted to the circuit arrangement using crystallisation of amorphous semiconductor or recrystallisation of crystalline semiconductor using control of the annealing or irradiation parameters, e.g. using different scanning direction or intensity for different transistors
Definitions
- the present disclosure relates to a method for manufacturing a semiconductor film.
- a laser annealing method is known as a method for manufacturing a semiconductor film of a Thin Film Transistor (TFT) used for a screen of a display such as a liquid crystal display or an organic EL (Electro Luminescence) display.
- TFT Thin Film Transistor
- an amorphous semiconductor film formed over a substrate is irradiated with a laser beam to be crystallized, so that a polycrystalline semiconductor film is formed.
- An Excimer Laser Anneal (hereinafter referred to as an ELA) apparatus that generates a laser beam using a mixed gas such as a rare gas and halogen is known as a laser annealing apparatus used in the laser annealing method.
- ELA apparatus Use of the ELA apparatus is widespread, because the ELA apparatus can obtain crystal grains with a substantially uniform size, i.e., high crystalline quality, when an amorphous semiconductor film is crystallized.
- high crystalline quality of a crystallized semiconductor film means that crystal grains are substantially uniform in size.
- the ELA apparatus has a problem that running cost is high.
- a solid-state laser using a solid material is known as a laser other than an excimer laser.
- the running cost of a laser annealing apparatus using a solid-state laser is lower than that of an ELA apparatus.
- a laser annealing apparatus using a solid-state laser has a problem that a semiconductor film with high crystalline quality cannot be formed stably as compared with that formed by an ELA apparatus.
- Japanese Unexamined Patent Application Publication No. 2017-224708 discloses a method for manufacturing a semiconductor film for forming a semiconductor film with high crystalline quality using a solid-state laser. According to the manufacturing method disclosed in Japanese Unexamined Patent Application Publication No. 2017-224708, first, a semiconductor film is irradiated with a first laser beam emitted from a solid-state laser. After that, the semiconductor film is irradiated with a second laser beam having the same intensity as that of the first laser beam.
- An example aspect of the present disclosure is a method for manufacturing a semiconductor film including a step of irradiating an amorphous semiconductor film with a first pulsed laser beam emitted from a solid-state laser, and a step of, after the above step, irradiating the semiconductor film with a second pulsed laser beam emitted from a solid-state laser and including intensity lower than that of the first pulsed laser beam.
- FIG. 1 shows an example of a pulse waveform of a laser beam emitted from an excimer laser
- FIG. 2 shows an example of a pulse waveform of a laser beam emitted from a solid-state laser
- FIG. 3 shows an example of an SEM photograph of a surface of a polysilicon film manufactured using an excimer laser
- FIG. 4 shows an example of an SEM photograph of a surface of a polysilicon film manufactured using a solid-state laser
- FIG. 5A is a cross-sectional view for describing an example of a state of a semiconductor film during laser annealing processing using an excimer laser;
- FIG. 5B is a cross-sectional view for describing an example of a state of a semiconductor film during laser annealing processing using an excimer laser;
- FIG. 6 shows an example of a pulse waveform of a laser beam used in the method for manufacturing a semiconductor film according to a first embodiment
- FIG. 7 is a flowchart showing an example of the method for manufacturing a semiconductor film according to the first embodiment
- FIG. 8 shows another example of the pulse waveform of the laser beam used in the method for manufacturing a semiconductor film according to the first embodiment
- FIG. 9 shows yet another example of the pulse waveform of the laser beam used in the method for manufacturing a semiconductor film according to the first embodiment
- FIG. 10 shows a configuration example of a laser processing apparatus according to a second embodiment
- FIG. 11 is a schematic diagram for describing an example of a laser beam applied to a semiconductor film in the laser processing apparatus according to the second embodiment
- FIG. 12 shows a configuration example of a laser processing apparatus according to a third embodiment
- FIG. 13 shows a configuration example of a laser processing apparatus according to a fourth embodiment
- FIG. 14 shows a configuration example of a laser annealing apparatus according to a fifth embodiment
- FIG. 15 is a schematic diagram for describing an example of a laser beam applied to a semiconductor film in the laser annealing apparatus according to the fifth embodiment
- FIG. 16 is a cross-sectional view showing an example of a method for manufacturing a semiconductor apparatus according to a sixth embodiment
- FIG. 17 is a cross-sectional view showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment.
- FIG. 18 is a cross-sectional view showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment.
- FIG. 19 is a cross-sectional view showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment.
- FIG. 20 is a cross-sectional view showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment.
- the polarization state of a laser beam emitted from an excimer laser is random polarized light (non-polarized light).
- the polarization state of a laser beam emitted from a solid-state laser is linearly polarized light.
- FIG. 1 shows an example of a pulse waveform of a laser beam emitted from an excimer laser.
- FIG. 2 shows an example of a pulse waveform of a laser beam emitted from a solid-state laser.
- the horizontal axis represents time
- the vertical axis represents intensity.
- the pulse waveform of the laser beam emitted from the excimer laser has two peaks P 1 and P 2 appearing consecutively.
- the pulse waveform is such that the peak P 2 that appears secondly has intensity lower than that of the peak P 1 that appears first.
- This pulse waveform is a pulse waveform unique to an excimer laser.
- the pulse waveform of the laser beam emitted from the solid-state laser has only one peak P appears.
- a surface state of a polysilicon film (p-Si film) obtained by irradiating an amorphous silicon film (a-Si film) formed over a substrate with a laser beam composed of a line beam using an excimer laser or a solid-state laser to crystallize the film will be described.
- FIG. 3 shows an example of an SEM (Scanning Electron Microscope) photograph of a surface of a polysilicon film manufactured using an excimer laser.
- FIG. 4 shows an example of an SEM photograph of a surface of a polysilicon film manufactured using a solid-state laser.
- parts that look whitish correspond to projections projecting from the surface, and black lines in the gaps between the projections correspond to grain boundaries that are boundaries between crystal grains.
- An excimer laser requires regular gas exchange about once every few days, because it uses a mixed gas such as a rare gas and halogen. Such a mixed gas is expensive. For this reason, the excimer laser has problems that maintainability is poor and running cost is high.
- a solid-state laser does not require gas exchange, because it does not need to use a mixed gas, unlike the excimer laser.
- the solid-state laser thus has an advantage, as compared with the excimer laser, that maintainability is good and running cost is low.
- the excimer laser has an advantage that a semiconductor film with high crystalline quality can be formed stably, but also has a problem that maintainability is poor and running cost is high.
- the solid-state laser has advantages that maintainability is good and running cost is low, but also has a problem that a semiconductor film with high crystalline quality cannot be formed stably.
- the present inventors have found that a pulse waveform unique to an excimer laser, in which two peaks P 1 and P 2 consecutively appear, and the intensity of the second peak P 2 is lower than that of the first peak P 1 , greatly contributes to achieving high crystalline quality of a crystallized semiconductor film. The reason for this will be described below.
- FIGS. 5A and 5B are cross-sectional views showing an example of a state of a semiconductor film M during laser annealing processing using an excimer laser 80 .
- the semiconductor film M is a silicon film.
- the semiconductor film M formed over a substrate S is irradiated with a laser beam composed of a line beam from the excimer laser 80 , and an amorphous silicon film is crystallized to form a polysilicon film.
- a part of the semiconductor film M irradiated with the laser beam from the excimer laser 80 is referred to as an irradiated part Ml
- a part of the semiconductor film M not irradiated with the laser beam from the excimer laser 80 is referred to as a non-irradiated part M 2
- a part of the irradiated part M 1 melted by the irradiation of the laser beam is referred to as a melted part M 11
- a part of the irradiated part M 1 not melted by the irradiation of the laser beam is referred to as a solid phase part M 12 .
- a high temperature part of the melted part M 11 is referred to as a high temperature part M 11 H
- a low temperature part of the melted part M 11 is referred to as a low temperature part M 11 L
- a high temperature part of the solid phase part M 12 is referred to as a high temperature part M 12 H
- a low temperature part of the solid phase part M 12 is referred to as a low temperature part M 12 L.
- the solid phase part M 12 becomes a nucleus, and crystals grow from the low temperature part M 12 L toward the high temperature part M 12 H with the nucleus as a starting point.
- the crystallized semiconductor film M has substantially uniform crystal grain size and high crystalline quality.
- the pulse waveform of the laser beam emitted from the excimer laser 80 has two peaks P 1 and P 2 appearing consecutively, and the intensity of the second peak P 2 is lower than that of the first peak P 1 .
- the laser beam of the excimer laser 80 is applied to the irradiated part M 1 of the semiconductor film M, first, the first peak P 1 of the laser beam is applied to the irradiated part M 1 , and the temperature of the upper layer part of the irradiated part M 1 gradually increases.
- the temperature of the upper layer part of the irradiated part M 1 becomes the melting point or higher, the upper layer part of the irradiated part M 1 is melted to form the melted part M 11 .
- the temperature of the melted part M 11 decreases.
- the irradiated part M 1 is not uniformly heated by the irradiation of the second peak P 2 . This may cause the size of the crystal grains to be inconsistent.
- a delay time from when the peak P 1 is applied until the peak P 2 is applied is considered to be such a delay time that the peak P 2 is applied before the melted part M 11 melted by the irradiation of the peak P 1 is solidified.
- the peak P 2 when the peak P 2 is applied before the melted part M 11 is solidified, the temperature of the melted part M 1 at that point does not decrease to the freezing point, and maintains at a high temperature. Therefore, if the peak P 2 has the same intensity as that of the first peak P 1 , the irradiation of the peak P 2 may cause the melting of the irradiated part M 1 to proceed, and the irradiated part M 1 may be completely melted.
- the intensity of the peak P 2 of the laser beam of the excimer laser 80 is lower than the intensity of the first peak P 1 .
- the irradiated part M 1 is not completely melted even by the irradiation of the peak P 2 , and the state in which only the upper layer part of the irradiated part M 1 is melted is maintained, as shown in FIGS. 5A and 5B .
- the semiconductor film M manufactured using the excimer laser 80 has substantially uniform crystal grain size and high crystalline quality.
- a pulse waveform of a laser beam unique to an excimer laser in which two peaks P 1 and P 2 consecutively appear, and the intensity of the second peak P 2 is lower than that of the first peak P 1 , greatly contributes to high crystalline quality of the semiconductor film M manufactured using an excimer laser.
- a solid-state laser is more advantageous than an excimer laser in terms of maintainability and running cost.
- a method for manufacturing the semiconductor film M according to the first embodiment is based on the above findings.
- the method for manufacturing the semiconductor film M according to the first embodiment uses a solid-state laser that is advantageous in terms of maintainability and running cost, and reproduces the pulse waveform unique to an excimer laser in order to achieve high crystalline quality of the semiconductor film, improve maintainability, and lower the running cost.
- FIG. 6 shows an example of a pulse waveform of a laser beam used in the method for manufacturing the semiconductor film M according to the first embodiment.
- the horizontal axis represents time
- the vertical axis represents intensity.
- two pulsed laser beams L 1 and L 2 emitted from a solid-state laser are multiplexed so that they become a pulse waveform similar to the pulse waveform ( FIG. 1 ) of the laser beam unique to the excimer laser. That is, the laser beams are multiplexed in such a way that two pulsed laser beams L 1 and L 2 become continuous, and the intensity of the second laser beam L 2 becomes lower than that of the first laser beam L 1 .
- FIG. 7 is a flowchart showing an example of the method for manufacturing the semiconductor film M according to the first embodiment.
- the amorphous semiconductor film M is irradiated with the pulsed laser beam L 1 emitted from the solid-state laser (Step S 1 ).
- the pulsed laser beam L 2 which is emitted from the solid-state laser and has intensity lower than that of the laser beam L 1 (Step S 2 ).
- a pulse waveform similar to the pulse waveform ( FIG. 1 ) of the laser beam unique to the excimer laser as shown in FIG. 6 is reproduced.
- the semiconductor film M manufactured by the manufacturing method according to the first embodiment is not completely melted even when irradiated with the laser beam L 2 subsequent to the irradiation with the laser beam L 1 , and as shown in FIGS. 5A and 5B , the state in which only the upper layer part of the semiconductor film M is melted is maintained for a certain time. As a result, the semiconductor film M having uniform crystal grain size and high crystalline quality can be formed.
- the semiconductor film M is not limited to the above-described silicon film and instead may be, for example, a germanium film.
- the solid-state laser may be, for example, a YAG (Yttrium Aluminum Garnet) laser or a YVO (Yttrium Vanadium Oxide) laser.
- a YAG Yttrium Aluminum Garnet
- a YVO Yttrium Vanadium Oxide
- the solid-state laser serving as a laser light source of the laser beams L 1 and L 2 may be separate solid-state lasers for the laser beams L 1 and L 2 or a single solid-state laser for both of the laser beams L 1 and L 2 .
- the polarization states of the laser beams L 1 and L 2 emitted from the solid-state laser are linearly polarized light.
- one or both of the laser beams L 1 and L 2 may be orthogonal linearly polarized light.
- the semiconductor film M may be irradiated with the laser beams L 1 and L 2 after the laser beams L 1 and L 2 are converted from linearly polarized light into circularly polarized light.
- any well-known method such as the method of using a polarizing mirror may be used.
- a method for making intensity of the laser beam L 1 differ from that of the laser beam L 2 may be any method.
- the difference between the intensity of the laser beam L 1 and that of the laser beam L 2 may be created by making the transmittance of a reflection mirror disposed over the optical path of one of the laser beams L 1 and L 2 different from the transmittance of a reflection mirror disposed over the optical path of the other one of the laser beams L 1 and L 2 .
- the difference between the intensity of the laser beam L 1 and that of the laser beam L 2 may be created by disposing an attenuator over the optical path of each of the laser beam L 1 and the laser beam L 2 .
- the difference between the intensity of the laser beam L 1 and that of the laser beam L 2 may be created by using different solid-state lasers with intensity different from each other for the laser beams L 1 and L 2 .
- the irradiation with the laser beam L 2 may be performed after a predetermined delay time has elapsed from the irradiation with the laser beam L 1 .
- the delay time at this time is preferably defined in such a way that the semiconductor film M is irradiated with the laser beam L 2 before the semiconductor film M melted by the irradiation of the laser beam L 1 is solidified.
- the semiconductor film M is uniformly heated by the irradiation of the laser beam L 2 , thereby contributing to high crystalline quality of the semiconductor film M.
- the laser beam applied to the semiconductor film M is not limited to the two laser beams L 1 and L 2 and instead may be three or more laser beams.
- a laser beam(s) other than the laser beams L 1 and L 2 may be applied from the solid-state laser.
- FIG. 8 shows an example in which a single pulsed laser beam L 3 is applied after the irradiation of the laser beam L 2 .
- FIG. 9 shows an example in which a plurality of pulsed laser beams L 3 (two laser beams L 3 in FIG. 9 ) are applied after the irradiation with the laser beam L 2 .
- the intensity of the laser beam L 3 is lower than the intensity of the laser beam L 2
- the intensity of the plurality of laser beams L 3 becomes gradually lower.
- the intensity of the laser beam L 3 only needs to be lower than that of the laser beam L 1 .
- the laser processing apparatus 1 is configured to multiplex two laser beams L 1 and L 2 (the same applies to a laser processing apparatus 101 in FIG. 12 and a laser processing apparatus 201 in FIG. 13 described below).
- FIG. 10 shows a configuration example of the laser processing apparatus 1 according to the second embodiment.
- the laser processing apparatus 1 is an apparatus for irradiating the semiconductor film M formed over a substrate with laser beams to crystallize the semiconductor film M.
- the semiconductor film M is irradiated with a laser beam composed of a line beam, and an amorphous silicon film is crystallized to form a polysilicon film.
- the laser processing apparatus 1 includes a solid-state laser 2 and an optical system module 10 .
- the solid-state laser 2 is a laser light source that generates pulsed laser beams by a pulse oscillation operation.
- the optical system module 10 includes an optical system casing 11 that constitutes an outer shape, optical elements such as a partial reflection mirror 3 , reflection mirrors 6 , and a homogenizer 4 , and a sealing window 23 . Laser beams generated by the solid-state laser 2 are guided to the partial reflection mirror 3 of the optical system module 10 .
- the partial reflection mirror 3 is composed of a first partial reflection mirror 3 a and a second partial reflection mirror 3 b.
- the first partial reflection mirror 3 a and the second partial reflection mirror 3 b are optical apparatuses configured to be able to change the transmittance, i.e., to be able to transmit some of the incident laser beams and reflect the rest.
- the partial reflection mirror 3 has a role of adjusting the timing at which the semiconductor film M is irradiated with a laser beam and adjusting the intensity of the laser beam.
- a laser beam emitted from the solid-state laser 2 is first guided to the first partial reflection mirror 3 a.
- the laser beam transmitted through the first partial reflection mirror 3 a is guided to the homogenizer 4 .
- the homogenizer 4 is composed of a plurality of cylindrical lenses and makes the intensity distribution uniform in a rectangular shape.
- the laser beam reflected by the first partial reflection mirror 3 a is reflected by the second partial reflection mirror 3 b, a direction of the laser beam is changed by the plurality of reflection mirrors 6 , and the laser beam is guided to the homogenizer 4 .
- the first optical path PT 1 is an optical path that guides a light beam transmitted through the first partial reflection mirror 3 a to the homogenizer 4
- the second optical path PT 2 is an optical path that guides a light beam reflected by the second partial reflection mirror 3 b to the homogenizer 4
- the second optical path PT 2 is longer than the first optical path PT 1 (second optical path PT 2 >first optical path PT 1 ).
- the laser beam (corresponding to the above-described laser beam L 1 ) first reaches the semiconductor film M through the first optical path PT 1 .
- the laser beam (corresponding to the above-described laser beam L 2 ) reaches the semiconductor film M through the second optical path PT 2 .
- the time interval (irradiation interval) at which the semiconductor film M is irradiated with the laser beams can be changed by making the length of the optical path variable.
- the intensity of the laser beam can be changed by changing the transmittance of the partial reflection mirror 3 . That is, by changing the transmittance of the first partial reflection mirror 3 a, the intensity of the laser beam (corresponding to the above-described laser beam L 1 ) through the first optical path PT 1 and the intensity the laser beam (corresponding to the above-described laser beam L 2 ) through the second optical path PT 2 can be changed.
- the semiconductor film M is disposed over a substrate stage 45 in a state in which the semiconductor film M is formed over a substrate (not shown).
- FIG. 11 is a schematic diagram for describing an example of a laser beam applied to the semiconductor film M.
- a laser beam L becomes a line beam after passing through the homogenizer 4 . That is, a cross section of the laser beam L orthogonal to an optical axis C is an elongated linear shape extending in one direction.
- a cross section of the laser beam L orthogonal to the optical axis reflected by the reflection mirror 6 is a linear shape extending in the Y-axis direction.
- the semiconductor film M is moved along the short axis direction (X-axis direction) of the line beam intermittently at a feed pitch of 5 to 10% of the short axis width of the line beam in one shot of the line beam.
- the feed pitch is 20 to 40 and the number of times of the amorphous silicon film is irradiated with laser beams per location is 10 to 20 times.
- the semiconductor film M is irradiated with a laser beam twice at different timings.
- the semiconductor film M is irradiated with the laser beams 14 times at different timings.
- the semiconductor film M is irradiated with the laser beams that have passed through the optical paths having different lengths, in accordance with the order of the respective lengths of the optical paths. That is, the semiconductor film M is irradiated firstly with the laser beam (corresponding to the above-described laser beam L 1 ) through the first optical path PT 1 having an optical path length shorter than that of the second optical path PT 2 . Then, the semiconductor film M is secondly irradiated with the laser beam (corresponding to the above-described laser beam L 2 ) through the second optical path PT 2 .
- the energy density of the laser beam (corresponding to the above-described laser beam L 1 ) that reaches the semiconductor film M first is defined as E 1
- the energy density of the laser beam (corresponding to the above-mentioned laser beam L 2 ) that reaches the semiconductor film M second is defined as E 2
- the reflectance of the first partial reflection mirror 3 a is defined as R 1
- the transmittance of the first partial reflection mirror 3 a is defined as T 1
- the reflectance of the second partial reflection mirror 3 b is defined as R 2 .
- the ratio r can be changed by appropriately changing R 1 , R 2 , and T 1 .
- the amorphous semiconductor film M is irradiated with the pulsed laser beam L 1 through the first optical path PT 1 .
- the semiconductor film M is irradiated with the laser beam L 2 through the second optical path PT 2 having intensity lower than that of the laser beam L 1 .
- a waveform similar to the pulse waveform ( FIG. 1 ) of the laser beam unique to the excimer laser is reproduced.
- the semiconductor film M having uniform crystal grain size and high crystalline quality can be formed.
- a laser processing apparatus 101 as another laser processing apparatus used in the above-described method for manufacturing the semiconductor film M according to the first embodiment will be described.
- FIG. 12 shows a configuration example of the laser processing apparatus 101 according to the third embodiment.
- the laser processing apparatus 101 further includes an attenuator 7 for attenuating a laser beam and adjusting the energy to predetermined energy density in addition to the components of the above-described laser processing apparatus 1 according to the second embodiment.
- an optical system module 110 includes the attenuator 7 as an optical element in addition to the partial reflection mirror 3 , the reflection mirror 6 , and the homogenizer 4 .
- the attenuator 7 is provided over the optical path between the solid-state laser 2 and the semiconductor film M.
- the attenuator 7 is disposed over each optical path (first optical path PT 1 and second optical path PT 2 ) leading from the first partial reflection mirror 3 a and the second partial reflection mirror 3 b to the homogenizer 4 .
- the attenuator 7 together with the partial reflection mirror 3 has a role of adjusting the intensity of the laser beam applied to the semiconductor film M. That is, the attenuator 7 and the partial reflection mirror 3 adjust the timing at which the semiconductor film M is irradiated with a laser beam next and adjust the intensity of this laser beam.
- the semiconductor film M when a laser beam is emitted once from the solid-state laser 2 , the semiconductor film M is irradiated with laser beams twice at different timings. For example, when the solid-state laser 2 emits a laser beam seven times, the semiconductor film M is irradiated with the laser beams 14 times at different timings.
- the semiconductor film M is firstly irradiated with the laser beam (corresponding to the above-described laser beam L 1 ) through the first optical path PT 1 having an optical path length longer than that of the second optical path PT 2 , and then secondly irradiated with the laser beam (corresponding to the above-described laser beam L 2 ) through the second optical path PT 2 .
- the energy density of the laser beam (corresponding to the above-described laser beam L 1 ) that reaches the semiconductor film M first is defined as E 1
- the energy density of the laser beam (corresponding to the above-mentioned laser beam L 2 ) that reaches the semiconductor film M second is defined as E 2
- the reflectance of the first partial reflection mirror 3 a is defined as R 1
- the transmittance of the first partial reflection mirror 3 a is defined as T 1
- the reflectance of the second partial reflection mirror 3 b is defined as R 2 .
- An attenuation factor of an attenuator 7 a is defined as Ta 0
- an attenuation factor of an attenuator 7 b is defined as Ta 1
- an attenuation factor of an attenuator 7 c is defined as Ta 2 .
- E 1 and E 2 are respectively expressed by the following formulas.
- the ratio r can be changed by appropriately changing R 1 , R 2 , T 1 , Ta 1 , and Ta 2 .
- the intensity of the laser beam is adjusted only by changing the transmittance of the partial reflection mirror 3 .
- the intensity of the laser beam is finely adjusted by the attenuators 7 disposed over the first optical path PT 1 and the second optical path PT 2 in addition to changing the transmittance of the partial reflection mirror 3 . By doing so, it is possible to adjust the intensity of a laser beam more accurately.
- the method for manufacturing the semiconductor film M in the laser processing apparatus 101 according to the third embodiment is the same as the above-described method for manufacturing the semiconductor film M in the laser processing apparatus 1 according to the second embodiment, and thus a description thereof is omitted.
- a laser processing apparatus 201 as another laser processing apparatus used in the method for manufacturing the semiconductor film M according to the first embodiment will be described.
- FIG. 13 shows a configuration example of the laser processing apparatus 201 according to the fourth embodiment.
- the laser processing apparatus 201 according to the fourth embodiment includes a plurality of solid-state lasers 2 (solid-state lasers 2 a and 2 b ).
- the laser processing apparatus 201 according to the fourth embodiment further includes a pulse generator 8 for applying laser beams from the plurality of solid-state lasers 2 a and 2 b with a time difference therebetween.
- the pulse generator 8 has a role of adjusting the timing of irradiating the semiconductor film M with laser beams.
- the laser beam emission timing of each of the solid-state lasers 2 a and 2 b is adjusted by the pulse generator 8 to thereby adjust an irradiation interval between a time when a laser beam is applied and a time when a laser beam is applied next.
- the laser processing apparatus 201 according to the fourth embodiment further includes, in an optical system module 210 , attenuators 7 for attenuating a laser beam and adjusting the energy to predetermined energy density in addition to optical elements such as the reflection mirror 6 and the homogenizer 4 .
- the attenuators 7 are provided in respective optical paths (first optical path PT 1 and second optical path PT 2 ) from the solid-state lasers 2 a and 2 b to the semiconductor film M.
- the attenuator 7 has a role of adjusting the intensity of the laser beam applied to the semiconductor film M. That is, the attenuator 7 and the pulse generator 8 adjust the timing at which the semiconductor film M is irradiated with a laser beam next and adjust the intensity of this laser beam. Note that the intensity of the laser beam applied to the semiconductor film M may be adjusted by making the intensity of the laser beams emitted from the solid-state lasers 2 a and 2 b different from each other.
- the semiconductor film M is irradiated with the laser beams twice at different timings.
- the semiconductor film M is irradiated with the laser beams 14 times at different timings.
- the pulse generator 8 adjusts the laser irradiation in such a way that the semiconductor film M is firstly irradiated with the laser beam (corresponding to the above-described laser beam L 1 ) through the first optical path PT 1 , and then the semiconductor film M is secondly irradiated with the laser beam (corresponding to the above-described laser beam L 2 ) through the second optical path PT 2 .
- the energy density of the laser beams emitted from the solid-state lasers 2 a and 2 b is defined as E 0
- the energy density of the laser beam reaching the semiconductor film M first is defined as E 1
- the energy density of the laser beam (corresponding to the above-described laser beam L 2 ) that reaches the semiconductor film M second is defined as E 2
- An attenuation factor of the attenuator 7 d is defined as Ta 3
- an attenuation factor of the attenuator 7 e is defined as Ta 4 .
- E 1 and E 2 are respectively expressed by the following formulas.
- the ratio r can be changed by appropriately changing Ta 3 and Ta 4 .
- the energy density of the laser beams emitted from the solid-state lasers 2 a and 2 b are both defined as E 0 .
- the ratio r can also be changed by making the energy density of the laser beams emitted from the solid-state lasers 2 a and 2 b different from each other.
- a laser beam emitted from the solid-state laser 2 needs to be divided by an optical system such as the partial reflection mirror 3 so that the divided laser beams pass through plurality of optical paths having different lengths to be applied to the semiconductor film M.
- the configuration of the optical system can be simpler, and thus the space required for disposing the optical system can be reduced, thereby reducing the apparatus size.
- the method for manufacturing the semiconductor film M in the laser processing apparatus 201 according to the fourth embodiment is the same as the above-described method for manufacturing the semiconductor film M in the laser processing apparatus 1 according to the second embodiment, and thus a description thereof is omitted.
- a laser annealing apparatus 301 as another laser processing apparatus used in the method for manufacturing the semiconductor film M according to the first embodiment will be described.
- the laser annealing apparatus 301 according to the fifth embodiment performs processing for irradiating the semiconductor film M formed over the substrate with a laser beam to crystallize the semiconductor film M.
- FIG. 14 shows a configuration example of the laser annealing apparatus 301 according to the fifth embodiment.
- the laser annealing apparatus 301 includes a solid-state laser 2 , an optical system module 20 , a sealing unit 30 , and a processing chamber 40 .
- the processing chamber 40 is provided, for example, over a horizontal base (not shown).
- the sealing unit 30 is provided above the processing chamber 40
- the optical system module 20 is provided above the sealing unit 30 .
- the optical system module 20 is provided at a position where the optical system module 20 can receive a laser beam L emitted from the solid-state laser 2 .
- XYZ orthogonal coordinate axes are introduced in order to describe the laser annealing apparatus 301 .
- the direction orthogonal to the upper surface of the horizontal base is defined as a Z-axis direction
- an upper direction of the Z-axis direction is defined as a +Z-axis direction
- a lower direction of the Z-axis direction is defined as a ⁇ Z-axis direction.
- the direction connecting the solid-state laser 2 to the optical system module 20 is defined as an X-axis direction
- a direction from the solid-state laser 2 toward the optical system module 20 is defined as a +X-axis direction
- a direction opposite to the +X-axis direction is defined as a ⁇ X-axis direction.
- a direction orthogonal to the X-axis direction and the Z-axis direction is defined as a Y-axis direction
- one direction of the Y-axis direction is defined as a +Y-axis direction
- a direction opposite to the +Y-axis direction is defined as a ⁇ Y-axis direction.
- the solid-state laser 2 is a laser light source that emits the laser beam L.
- the solid-state laser 2 is, for example, a YAG laser or a YVO laser.
- the solid-state laser 2 emits the laser beam L toward the optical system module 20 .
- the laser beam L travels, for example, in the +X-axis direction and enters the optical system module 20 .
- the optical system module 20 includes an optical system casing 21 that constitutes an outer shape, optical elements such as a reflection mirror 6 , and a sealing window 23 .
- the optical system casing 21 is a box-shaped member made of a material such as aluminum.
- Each optical element of the optical system module 20 is held inside the optical system casing 21 by a holder or the like. With such optical elements, the optical system module 20 adjusts the irradiation direction, the light amount, and the like of the laser beam L emitted from the solid-state laser 2 .
- the configuration of the above-described optical system module 10 of the laser processing apparatus 1 according to the second embodiment is applied as a configuration of the optical system module 20 .
- the configuration of the above-described optical system module 110 of the laser processing apparatus 101 according to the third embodiment or the above-described configuration of the laser processing apparatus 201 of the optical system module 210 according to the fourth embodiment may be applied as the configuration of the optical module 20 .
- the sealing window 23 is provided over a part of the optical system casing 21 , for example, over a lower surface of the optical system casing 21 .
- FIG. 15 is a schematic diagram showing an example of a laser beam applied to the semiconductor film M.
- the laser beam L has a line beam shape in the optical system module 20 . That is, the cross section of the laser beam L orthogonal to an optical axis C is an elongated linear shape extending in one direction.
- a cross section of the laser beam L orthogonal to the optical axis of the laser beam L reflected by the reflection mirror 6 is a linear shape extending in the Y-axis direction.
- the sealing unit 30 includes a sealing casing 31 , a reflected light receiving member 61 , a sealing window 33 , a gas inlet 34 , and a gas outlet 35 .
- the sealing casing 31 is a box-shaped member with a hollow inside.
- Each of the gas inlet 34 and the gas outlet 35 is provided over a predetermined side surface of the sealing casing 31 .
- the gas inlet 34 and the gas outlet 35 are provided, for example, over side surfaces of the sealing casing 31 opposite to each other.
- the gas outlet 35 is provided above the gas inlet 34 .
- a gas 37 for example, an inert gas such as nitrogen is introduced from the gas inlet 34 .
- the gas 37 introduced inside the sealing casing 31 from the gas inlet 34 is discharged from the gas outlet 35 . It is desirable that the gas 37 be continuously supplied inside the sealing casing 31 . Further, it is desirable that the gas 37 be continuously discharged to the outside of the sealing casing 31 .
- a flow rate of the gas 37 is controlled to a predetermined flow rate so that the inside of the sealing casing 31 is constantly ventilated.
- the reflected light receiving member 61 is disposed inside the sealing casing 31 .
- the reflected light receiving member 61 is disposed outside the optical system module 20 in such a way that the reflected light receiving member 61 is spaced from the optical system module 20 .
- the reflected light receiving member 61 is, for example, a plate-shaped member.
- the reflected light receiving member 61 is disposed with a plate surface facing the Z-axis direction.
- the reflected light receiving member 61 is disposed in such a way that it can receive a reflected beam R of the laser beam L reflected to the semiconductor film M.
- the reflected light receiving member 61 is disposed over the optical path of the reflected beam R in consideration of an incident angle of the laser beam L and a reflection angle of the reflected beam R.
- the reflected light receiving member 61 may be attached to the optical system module 20 with a heat insulating material 62 and a space therebetween. By doing so, heat insulation between the reflected light receiving member 61 and the optical system module 20 can be maintained.
- the sealing window 33 is provided over a part of the sealing casing 31 , for example, over a lower surface of the sealing casing 31 .
- the laser beam L emitted from the sealing window 23 of the optical system module 20 is emitted from the sealing window 33 of the sealing unit 30 toward the processing chamber 40 .
- the processing chamber 40 includes a gas box 41 , a substrate stage 45 , a substrate base 46 , and a scanning apparatus 47 .
- the semiconductor film M is disposed over the substrate stage 45 in a state in which the semiconductor film M is formed over a substrate (not shown).
- the semiconductor film M disposed over the substrate stage 45 is irradiated with the laser beam L and then subject to laser annealing processing for crystallizing the semiconductor film M.
- the substrate stage 45 may be a float type stage, i.e., a stage that transports the substrate over which the semiconductor film M is formed while the substrate is floated.
- the gas box 41 is a box-shaped member with a hollow inside.
- the gas box 41 is disposed above the substrate stage 45 and below the sealing window 33 in the sealing unit 30 .
- An introduction window 42 is provided over an upper surface of the gas box 41 .
- the introduction window 42 is disposed to face the sealing window 33 .
- An irradiation window 43 is provided over a lower surface of the gas box 41 .
- the irradiation window 43 is disposed to face the semiconductor film M.
- a gas inlet 44 is provided over a predetermined side surface of the gas box 41 .
- a predetermined gas 37 for example, an inert gas such as nitrogen is supplied to the gas box 41 from the gas inlet 44 . After the inside of the gas box 41 is filled with the gas 37 supplied to the gas box 41 , the gas 37 is discharged from the irradiation window 43 .
- the laser beam L incident over the gas box 41 is emitted from the irradiation window 43 and applied to the semiconductor film M.
- the reflected light receiving member 61 is disposed in such a way that it can receive the reflected beam R reflected by the semiconductor film M of the laser beam L applied to the semiconductor film M.
- the substrate stage 45 is disposed over the scanning apparatus 47 with, for example, a substrate base 46 interposed therebetween.
- the substrate stage 45 can be moved by the scanning apparatus 47 in the X-axis direction, the Y-axis direction, and the Z-axis direction.
- the substrate stage 45 is transported by the scanning of the scanning apparatus 47 , for example, in a transport direction 48 in the ⁇ X-axis direction.
- the method for manufacturing the semiconductor film M in the laser annealing apparatus 301 according to the fifth embodiment is the same as the above-described method for manufacturing the semiconductor film M in the laser processing apparatus 1 according to the second embodiment, and thus a description thereof is omitted.
- the above-described laser annealing apparatus 301 according to the fifth embodiment is used as a laser processing apparatus.
- the method for manufacturing a semiconductor apparatus according to the sixth embodiment includes a step of preparing an object to be processed including a substrate and an amorphous semiconductor film formed over the substrate and a step of irradiating the semiconductor film with a laser beam and crystallizing the semiconductor film.
- a substrate over which an amorphous semiconductor film is formed for example, a glass substrate over which amorphous silicon is formed, is used.
- laser annealing processing using the above-described laser annealing apparatus 301 according to the fifth embodiment is performed.
- the semiconductor apparatus includes a TFT (Thin Film Transistor).
- TFT Thin Film Transistor
- an amorphous silicon film is irradiated with a laser beam and then crystallized, so that a polysilicon film is formed.
- FIGS. 16 to 20 are cross-sectional views showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment.
- the above-described laser annealing apparatus 301 according to the sixth embodiment is suitable for manufacturing a TFT array substrate.
- a method for manufacturing a semiconductor apparatus including a TFT will be described.
- a gate electrode 92 is formed over a glass substrate 91 .
- a metal thin film containing aluminum or the like can be used as the gate electrode 92 .
- a gate insulating film 93 is formed over the gate electrode 92 .
- the gate insulating film 93 is formed to cover the gate electrode 92 .
- an amorphous silicon film 94 is formed over the gate insulating film 93 .
- the amorphous silicon film 94 is disposed to overlap the gate electrode 92 with the gate insulating film 93 interposed therebetween.
- the gate insulating film 93 is a silicon nitride film (SiN x ), a silicon oxide film (SiO 2 film), or a laminated film of these, etc. Specifically, the gate insulating film 93 and the amorphous silicon film 94 are continuously formed by a CVD (Chemical Vapor Deposition) method. The amorphous silicon film 94 becomes the semiconductor film M in the laser processing apparatus.
- the amorphous silicon film 94 is irradiated with a laser beam to crystallize the amorphous silicon film 94 using the above-described laser annealing apparatus 301 according to the fifth embodiment, so that a polysilicon film 95 is formed.
- a first position control signal for controlling a disposed position of the substrate over the substrate stage 45 is transmitted to a loading/unloading apparatus (not shown) that loads and unloads the substrate (Step B).
- the substrate is disposed by the loading/unloading apparatus at a first position over the substrate stage 45 determined by the first position control signal (Step C).
- the substrate is transported over the substrate stage 45 (Step D), and the substrate is irradiated with a laser beam to polycrystallize an amorphous semiconductor film (Step E). After the amorphous semiconductor film is polycrystallized, the substrate is unloaded by the loading/unloading apparatus (Step F).
- a second position control signal is further transmitted to the loading/unloading apparatus (Step G), and the substrate is disposed by the loading/unloading apparatus to a second position different from the first position over the substrate stage 45 determined by the second position control signal (Step H). Then, the substrate is transported to a laser beam irradiation position over the substrate stage 45 (Step I), and the substrate is irradiated with a laser beam (Step J). Then, the polysilicon film 95 in which silicon is crystallized is formed over the gate insulating film 93 .
- the pulsed laser beam L 1 from the solid-state laser 2 is applied, and after that, the pulsed laser beam L 2 having intensity lower than that of the laser beam L 1 is applied from the solid-state laser 2 .
- a waveform similar to the pulse waveform ( FIG. 1 ) of the laser beam unique to the excimer laser is reproduced.
- the semiconductor film M having uniform crystal grain size and high crystalline quality can be formed. Further, since a solid-state laser is used, maintainability is improved, and running cost can be reduced.
- Step K After all the irradiation areas are irradiated and the semiconductor film is polycrystallized, the substrate is unloaded by the loading/unloading apparatus (Step K).
- an interlayer insulating film 96 , a source electrode 97 a, and a drain electrode 97 b are formed over the polysilicon film 95 .
- the interlayer insulating film 96 , the source electrode 97 a, and the drain electrode 97 b can be formed by using a common photolithography method or film forming method.
- a semiconductor apparatus provided with a TFT including a polycrystalline semiconductor film can be manufactured using the method for manufacturing a semiconductor apparatus according to the sixth embodiment.
- Such a semiconductor apparatus may be used for a screen of a display such as a liquid crystal display. Note that the subsequent manufacturing steps differ depending on the device to be eventually manufactured, and thus the description of the subsequent manufacturing steps will be omitted.
- the first to sixth embodiments can be combined as desirable by one of ordinary skill in the art.
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Abstract
Description
- This application is based upon and claims the benefit of priority from Japanese patent application No. 2019-084976, filed on Apr. 26, 2019, the disclosure of which is incorporated herein in its entirety by reference.
- The present disclosure relates to a method for manufacturing a semiconductor film.
- A laser annealing method is known as a method for manufacturing a semiconductor film of a Thin Film Transistor (TFT) used for a screen of a display such as a liquid crystal display or an organic EL (Electro Luminescence) display. In the laser annealing method, an amorphous semiconductor film formed over a substrate is irradiated with a laser beam to be crystallized, so that a polycrystalline semiconductor film is formed.
- An Excimer Laser Anneal (hereinafter referred to as an ELA) apparatus that generates a laser beam using a mixed gas such as a rare gas and halogen is known as a laser annealing apparatus used in the laser annealing method. Use of the ELA apparatus is widespread, because the ELA apparatus can obtain crystal grains with a substantially uniform size, i.e., high crystalline quality, when an amorphous semiconductor film is crystallized. Hereinafter, high crystalline quality of a crystallized semiconductor film means that crystal grains are substantially uniform in size.
- However, the ELA apparatus has a problem that running cost is high. A solid-state laser using a solid material is known as a laser other than an excimer laser. The running cost of a laser annealing apparatus using a solid-state laser is lower than that of an ELA apparatus. However, a laser annealing apparatus using a solid-state laser has a problem that a semiconductor film with high crystalline quality cannot be formed stably as compared with that formed by an ELA apparatus.
- Japanese Unexamined Patent Application Publication No. 2017-224708 discloses a method for manufacturing a semiconductor film for forming a semiconductor film with high crystalline quality using a solid-state laser. According to the manufacturing method disclosed in Japanese Unexamined Patent Application Publication No. 2017-224708, first, a semiconductor film is irradiated with a first laser beam emitted from a solid-state laser. After that, the semiconductor film is irradiated with a second laser beam having the same intensity as that of the first laser beam.
- However, the present inventors have found through studies that forming a semiconductor film with high crystalline quality could be further improved using a solid-state laser.
- Other problems and novel features will be apparent from the description of the present specification and the attached drawings.
- An example aspect of the present disclosure is a method for manufacturing a semiconductor film including a step of irradiating an amorphous semiconductor film with a first pulsed laser beam emitted from a solid-state laser, and a step of, after the above step, irradiating the semiconductor film with a second pulsed laser beam emitted from a solid-state laser and including intensity lower than that of the first pulsed laser beam.
- According to the above example aspect, it is possible to provide a method for manufacturing a semiconductor film capable of forming a semiconductor film with high crystalline quality using a solid-state laser.
- The above and other objects, features and advantages of the present disclosure will become more fully understood from the detailed description given hereinbelow and the accompanying drawings which are given by way of illustration only, and thus are not to be considered as limiting the present disclosure.
-
FIG. 1 shows an example of a pulse waveform of a laser beam emitted from an excimer laser; -
FIG. 2 shows an example of a pulse waveform of a laser beam emitted from a solid-state laser; -
FIG. 3 shows an example of an SEM photograph of a surface of a polysilicon film manufactured using an excimer laser; -
FIG. 4 shows an example of an SEM photograph of a surface of a polysilicon film manufactured using a solid-state laser; -
FIG. 5A is a cross-sectional view for describing an example of a state of a semiconductor film during laser annealing processing using an excimer laser; -
FIG. 5B is a cross-sectional view for describing an example of a state of a semiconductor film during laser annealing processing using an excimer laser; -
FIG. 6 shows an example of a pulse waveform of a laser beam used in the method for manufacturing a semiconductor film according to a first embodiment; -
FIG. 7 is a flowchart showing an example of the method for manufacturing a semiconductor film according to the first embodiment; -
FIG. 8 shows another example of the pulse waveform of the laser beam used in the method for manufacturing a semiconductor film according to the first embodiment; -
FIG. 9 shows yet another example of the pulse waveform of the laser beam used in the method for manufacturing a semiconductor film according to the first embodiment; -
FIG. 10 shows a configuration example of a laser processing apparatus according to a second embodiment; -
FIG. 11 is a schematic diagram for describing an example of a laser beam applied to a semiconductor film in the laser processing apparatus according to the second embodiment; -
FIG. 12 shows a configuration example of a laser processing apparatus according to a third embodiment; -
FIG. 13 shows a configuration example of a laser processing apparatus according to a fourth embodiment; -
FIG. 14 shows a configuration example of a laser annealing apparatus according to a fifth embodiment; -
FIG. 15 is a schematic diagram for describing an example of a laser beam applied to a semiconductor film in the laser annealing apparatus according to the fifth embodiment; -
FIG. 16 is a cross-sectional view showing an example of a method for manufacturing a semiconductor apparatus according to a sixth embodiment; -
FIG. 17 is a cross-sectional view showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment; -
FIG. 18 is a cross-sectional view showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment; -
FIG. 19 is a cross-sectional view showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment; and -
FIG. 20 is a cross-sectional view showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment. - Hereinafter, specific embodiments of the present disclosure will be described in detail with reference to the drawings. However, the present disclosure is not limited to the following embodiments. In addition, the following description and drawings are simplified as appropriate for clarity of descriptions. The same elements are denoted by the same reference signs throughout the drawings, and repeated description is omitted as necessary.
- Prior to describing the embodiments of the present disclosure, an excimer laser and a solid-state laser will be described in comparison with each other.
- The polarization state of a laser beam emitted from an excimer laser is random polarized light (non-polarized light).
- On the other hand, the polarization state of a laser beam emitted from a solid-state laser is linearly polarized light.
-
FIG. 1 shows an example of a pulse waveform of a laser beam emitted from an excimer laser.FIG. 2 shows an example of a pulse waveform of a laser beam emitted from a solid-state laser. InFIGS. 1 and 2 , the horizontal axis represents time, and the vertical axis represents intensity. - As shown in
FIG. 1 , the pulse waveform of the laser beam emitted from the excimer laser has two peaks P1 and P2 appearing consecutively. The pulse waveform is such that the peak P2 that appears secondly has intensity lower than that of the peak P1 that appears first. This pulse waveform is a pulse waveform unique to an excimer laser. - On the other hand, as shown in
FIG. 2 , the pulse waveform of the laser beam emitted from the solid-state laser has only one peak P appears. - Next, a surface state of a polysilicon film (p-Si film) obtained by irradiating an amorphous silicon film (a-Si film) formed over a substrate with a laser beam composed of a line beam using an excimer laser or a solid-state laser to crystallize the film will be described.
-
FIG. 3 shows an example of an SEM (Scanning Electron Microscope) photograph of a surface of a polysilicon film manufactured using an excimer laser.FIG. 4 shows an example of an SEM photograph of a surface of a polysilicon film manufactured using a solid-state laser. InFIGS. 3 and 4 , parts that look whitish correspond to projections projecting from the surface, and black lines in the gaps between the projections correspond to grain boundaries that are boundaries between crystal grains. - As shown in
FIG. 3 , it can be seen that in the polysilicon film manufactured using an excimer laser, projections are arranged at substantially equal intervals, crystal grains are substantially uniform in size, and crystal grains are arranged with regularity. This means that high crystalline quality is achieved. - On the other hand, as shown in
FIG. 4 , it can be seen that in the polysilicon film manufactured using a solid-state laser, as compared with the polysilicon film manufactured using the excimer laser, the projections are arranged irregularly, and there are many grain boundaries in the gaps between the projections. This means that high crystalline quality is not achieved. Such a polysilicon film is not suitable for a thin film transistor such as a liquid crystal display. - An excimer laser requires regular gas exchange about once every few days, because it uses a mixed gas such as a rare gas and halogen. Such a mixed gas is expensive. For this reason, the excimer laser has problems that maintainability is poor and running cost is high.
- On the other hand, a solid-state laser does not require gas exchange, because it does not need to use a mixed gas, unlike the excimer laser. The solid-state laser thus has an advantage, as compared with the excimer laser, that maintainability is good and running cost is low.
- As described above, the excimer laser has an advantage that a semiconductor film with high crystalline quality can be formed stably, but also has a problem that maintainability is poor and running cost is high.
- On the other hand, the solid-state laser has advantages that maintainability is good and running cost is low, but also has a problem that a semiconductor film with high crystalline quality cannot be formed stably.
- The present inventors have found that a pulse waveform unique to an excimer laser, in which two peaks P1 and P2 consecutively appear, and the intensity of the second peak P2 is lower than that of the first peak P1, greatly contributes to achieving high crystalline quality of a crystallized semiconductor film. The reason for this will be described below.
-
FIGS. 5A and 5B are cross-sectional views showing an example of a state of a semiconductor film M during laser annealing processing using anexcimer laser 80. In the example ofFIGS. 5A and 5B , the semiconductor film M is a silicon film. In manufacturing of the semiconductor film M, the semiconductor film M formed over a substrate S is irradiated with a laser beam composed of a line beam from theexcimer laser 80, and an amorphous silicon film is crystallized to form a polysilicon film. InFIGS. 5A and 5B , for convenience, a part of the semiconductor film M irradiated with the laser beam from theexcimer laser 80 is referred to as an irradiated part Ml, and a part of the semiconductor film M not irradiated with the laser beam from theexcimer laser 80 is referred to as a non-irradiated part M2. Further, a part of the irradiated part M1 melted by the irradiation of the laser beam is referred to as a melted part M11, and a part of the irradiated part M1 not melted by the irradiation of the laser beam is referred to as a solid phase part M12. A high temperature part of the melted part M11 is referred to as a high temperature part M11H, a low temperature part of the melted part M11 is referred to as a low temperature part M11L, and a high temperature part of the solid phase part M12 is referred to as a high temperature part M12H, and a low temperature part of the solid phase part M12 is referred to as a low temperature part M12L. - As shown in
FIG. 5A , when the irradiated part M1 of the semiconductor film M is irradiated with the laser beam from theexcimer laser 80, and an upper layer part of the irradiated part M1 is melted to become the melted part M11. Surface plasmons are generated over the surface of the melted part M11. - At this time, a standing wave is generated in the melted part M11, and a temperature distribution in which the high temperature part M11H and the low temperature part M11L periodically appear in the horizontal direction (film surface direction) is formed.
- When the state shown in
FIG. 5A is maintained, as shown inFIG. 5B the periodic temperature distribution of the melted part M11 is reflected to the solid phase part M12, a temperature distribution in which the high temperature part M12H and the low temperature part M12L periodically appear in the horizontal direction is formed also in the solid phase part M12. - Then, the solid phase part M12 becomes a nucleus, and crystals grow from the low temperature part M12L toward the high temperature part M12H with the nucleus as a starting point. As a result of such a solid phase growth process, the crystallized semiconductor film M has substantially uniform crystal grain size and high crystalline quality.
- Thus, it is necessary to ensure an enough time for growing crystals in the solid phase part M12 in order to form the semiconductor film M with high crystalline quality. In order to do so, as shown in
FIGS. 5A and 5B , it is important to maintain a state in which a melting depth of the semiconductor film M does not reach an interface between the irradiated part M1 and the substrate S, and only the melted part M11 in the upper layer part of the irradiated part M1 is melted, i.e., the state in which the irradiated part M1 of the semiconductor film M is not completely melted, for a certain period of time. - Here, as described with reference to
FIG. 1 , the pulse waveform of the laser beam emitted from theexcimer laser 80 has two peaks P1 and P2 appearing consecutively, and the intensity of the second peak P2 is lower than that of the first peak P1. - When the laser beam of the
excimer laser 80 is applied to the irradiated part M1 of the semiconductor film M, first, the first peak P1 of the laser beam is applied to the irradiated part M1, and the temperature of the upper layer part of the irradiated part M1 gradually increases. When the temperature of the upper layer part of the irradiated part M1 becomes the melting point or higher, the upper layer part of the irradiated part M1 is melted to form the melted part M11. - After that, the temperature of the melted part M11 decreases. When the temperature of the melted part M11 decreases to a freezing point and the melted part M11 is solidified, the irradiated part M1 is not uniformly heated by the irradiation of the second peak P2. This may cause the size of the crystal grains to be inconsistent. In such a case, a delay time from when the peak P1 is applied until the peak P2 is applied is considered to be such a delay time that the peak P2 is applied before the melted part M11 melted by the irradiation of the peak P1 is solidified.
- However, when the peak P2 is applied before the melted part M11 is solidified, the temperature of the melted part M1 at that point does not decrease to the freezing point, and maintains at a high temperature. Therefore, if the peak P2 has the same intensity as that of the first peak P1, the irradiation of the peak P2 may cause the melting of the irradiated part M1 to proceed, and the irradiated part M1 may be completely melted.
- However, as described with reference to
FIG. 1 , the intensity of the peak P2 of the laser beam of theexcimer laser 80 is lower than the intensity of the first peak P1. For this reason, the irradiated part M1 is not completely melted even by the irradiation of the peak P2, and the state in which only the upper layer part of the irradiated part M1 is melted is maintained, as shown inFIGS. 5A and 5B . As a result, it is considered that the semiconductor film M manufactured using theexcimer laser 80 has substantially uniform crystal grain size and high crystalline quality. - As described above, a pulse waveform of a laser beam unique to an excimer laser, in which two peaks P1 and P2 consecutively appear, and the intensity of the second peak P2 is lower than that of the first peak P1, greatly contributes to high crystalline quality of the semiconductor film M manufactured using an excimer laser.
- However, a solid-state laser is more advantageous than an excimer laser in terms of maintainability and running cost.
- A method for manufacturing the semiconductor film M according to the first embodiment is based on the above findings. The method for manufacturing the semiconductor film M according to the first embodiment uses a solid-state laser that is advantageous in terms of maintainability and running cost, and reproduces the pulse waveform unique to an excimer laser in order to achieve high crystalline quality of the semiconductor film, improve maintainability, and lower the running cost.
-
FIG. 6 shows an example of a pulse waveform of a laser beam used in the method for manufacturing the semiconductor film M according to the first embodiment. InFIG. 6 , the horizontal axis represents time, and the vertical axis represents intensity. - As shown in
FIG. 6 , in the method for manufacturing the semiconductor film M according to the first embodiment, two pulsed laser beams L1 and L2 emitted from a solid-state laser are multiplexed so that they become a pulse waveform similar to the pulse waveform (FIG. 1 ) of the laser beam unique to the excimer laser. That is, the laser beams are multiplexed in such a way that two pulsed laser beams L1 and L2 become continuous, and the intensity of the second laser beam L2 becomes lower than that of the first laser beam L1. -
FIG. 7 is a flowchart showing an example of the method for manufacturing the semiconductor film M according to the first embodiment. - As shown in
FIG. 7 , first, the amorphous semiconductor film M is irradiated with the pulsed laser beam L1 emitted from the solid-state laser (Step S1). Next, after the above semiconductor film M is irradiated with the laser beam L1, it is irradiated with the pulsed laser beam L2 which is emitted from the solid-state laser and has intensity lower than that of the laser beam L1 (Step S2). Then, a pulse waveform similar to the pulse waveform (FIG. 1 ) of the laser beam unique to the excimer laser as shown inFIG. 6 is reproduced. - Thus, the semiconductor film M manufactured by the manufacturing method according to the first embodiment is not completely melted even when irradiated with the laser beam L2 subsequent to the irradiation with the laser beam L1, and as shown in
FIGS. 5A and 5B , the state in which only the upper layer part of the semiconductor film M is melted is maintained for a certain time. As a result, the semiconductor film M having uniform crystal grain size and high crystalline quality can be formed. - Additionally, since a solid-state laser is used in the method for manufacturing the semiconductor film M according to the first embodiment, maintainability is improved, and running cost can be reduced.
- The semiconductor film M is not limited to the above-described silicon film and instead may be, for example, a germanium film.
- The solid-state laser may be, for example, a YAG (Yttrium Aluminum Garnet) laser or a YVO (Yttrium Vanadium Oxide) laser.
- The solid-state laser serving as a laser light source of the laser beams L1 and L2 may be separate solid-state lasers for the laser beams L1 and L2 or a single solid-state laser for both of the laser beams L1 and L2.
- The polarization states of the laser beams L1 and L2 emitted from the solid-state laser are linearly polarized light. However, one or both of the laser beams L1 and L2 may be orthogonal linearly polarized light. Alternatively, the semiconductor film M may be irradiated with the laser beams L1 and L2 after the laser beams L1 and L2 are converted from linearly polarized light into circularly polarized light. As a method for converting linearly polarized light into circularly polarized light, any well-known method such as the method of using a polarizing mirror may be used.
- Further, a method for making intensity of the laser beam L1 differ from that of the laser beam L2 may be any method. For example, the difference between the intensity of the laser beam L1 and that of the laser beam L2 may be created by making the transmittance of a reflection mirror disposed over the optical path of one of the laser beams L1 and L2 different from the transmittance of a reflection mirror disposed over the optical path of the other one of the laser beams L1 and L2. Alternatively, the difference between the intensity of the laser beam L1 and that of the laser beam L2 may be created by disposing an attenuator over the optical path of each of the laser beam L1 and the laser beam L2. Further alternatively, the difference between the intensity of the laser beam L1 and that of the laser beam L2 may be created by using different solid-state lasers with intensity different from each other for the laser beams L1 and L2.
- The irradiation with the laser beam L2 may be performed after a predetermined delay time has elapsed from the irradiation with the laser beam L1. The delay time at this time is preferably defined in such a way that the semiconductor film M is irradiated with the laser beam L2 before the semiconductor film M melted by the irradiation of the laser beam L1 is solidified. By avoiding the solidification of the semiconductor film M in this manner, the semiconductor film M is uniformly heated by the irradiation of the laser beam L2, thereby contributing to high crystalline quality of the semiconductor film M.
- The laser beam applied to the semiconductor film M is not limited to the two laser beams L1 and L2 and instead may be three or more laser beams. After the laser beam L2 is applied, a laser beam(s) other than the laser beams L1 and L2 may be applied from the solid-state laser.
FIG. 8 shows an example in which a single pulsed laser beam L3 is applied after the irradiation of the laser beam L2.FIG. 9 shows an example in which a plurality of pulsed laser beams L3 (two laser beams L3 inFIG. 9 ) are applied after the irradiation with the laser beam L2. InFIGS. 8 and 9 , the intensity of the laser beam L3 is lower than the intensity of the laser beam L2, and inFIG. 9 , the intensity of the plurality of laser beams L3 becomes gradually lower. However, the present disclosure is not limited to such cases. The intensity of the laser beam L3 only needs to be lower than that of the laser beam L1. - Next, as a second embodiment, a
laser processing apparatus 1 used in the above-described method for manufacturing the semiconductor film M according to the first embodiment will be described. Note that thelaser processing apparatus 1 is configured to multiplex two laser beams L1 and L2 (the same applies to alaser processing apparatus 101 inFIG. 12 and alaser processing apparatus 201 inFIG. 13 described below). -
FIG. 10 shows a configuration example of thelaser processing apparatus 1 according to the second embodiment. Thelaser processing apparatus 1 is an apparatus for irradiating the semiconductor film M formed over a substrate with laser beams to crystallize the semiconductor film M. Here, in manufacturing of the semiconductor film M, the semiconductor film M is irradiated with a laser beam composed of a line beam, and an amorphous silicon film is crystallized to form a polysilicon film. As shown inFIG. 10 , thelaser processing apparatus 1 includes a solid-state laser 2 and anoptical system module 10. - The solid-
state laser 2 is a laser light source that generates pulsed laser beams by a pulse oscillation operation. Theoptical system module 10 includes an optical system casing 11 that constitutes an outer shape, optical elements such as apartial reflection mirror 3, reflection mirrors 6, and ahomogenizer 4, and a sealingwindow 23. Laser beams generated by the solid-state laser 2 are guided to thepartial reflection mirror 3 of theoptical system module 10. Thepartial reflection mirror 3 is composed of a firstpartial reflection mirror 3 a and a secondpartial reflection mirror 3 b. The firstpartial reflection mirror 3 a and the secondpartial reflection mirror 3 b are optical apparatuses configured to be able to change the transmittance, i.e., to be able to transmit some of the incident laser beams and reflect the rest. Thepartial reflection mirror 3 has a role of adjusting the timing at which the semiconductor film M is irradiated with a laser beam and adjusting the intensity of the laser beam. - A laser beam emitted from the solid-
state laser 2 is first guided to the firstpartial reflection mirror 3 a. The laser beam transmitted through the firstpartial reflection mirror 3 a is guided to thehomogenizer 4. Thehomogenizer 4 is composed of a plurality of cylindrical lenses and makes the intensity distribution uniform in a rectangular shape. On the other hand, the laser beam reflected by the firstpartial reflection mirror 3 a is reflected by the secondpartial reflection mirror 3 b, a direction of the laser beam is changed by the plurality of reflection mirrors 6, and the laser beam is guided to thehomogenizer 4. - There is a difference between a length of a first optical path PT1 and a length of a second optical path PT2. The first optical path PT1 is an optical path that guides a light beam transmitted through the first
partial reflection mirror 3 a to thehomogenizer 4, while the second optical path PT2 is an optical path that guides a light beam reflected by the secondpartial reflection mirror 3 b to thehomogenizer 4. The second optical path PT2 is longer than the first optical path PT1 (second optical path PT2 >first optical path PT1). Thus, when a laser beam is emitted once from the solid-state laser 2, the laser beam (corresponding to the above-described laser beam L1) first reaches the semiconductor film M through the first optical path PT1. Next, the laser beam (corresponding to the above-described laser beam L2) reaches the semiconductor film M through the second optical path PT2. In this manner, the time interval (irradiation interval) at which the semiconductor film M is irradiated with the laser beams can be changed by making the length of the optical path variable. - Further, the intensity of the laser beam can be changed by changing the transmittance of the
partial reflection mirror 3. That is, by changing the transmittance of the firstpartial reflection mirror 3 a, the intensity of the laser beam (corresponding to the above-described laser beam L1) through the first optical path PT1 and the intensity the laser beam (corresponding to the above-described laser beam L2) through the second optical path PT2 can be changed. - The semiconductor film M is disposed over a
substrate stage 45 in a state in which the semiconductor film M is formed over a substrate (not shown). -
FIG. 11 is a schematic diagram for describing an example of a laser beam applied to the semiconductor film M. As shown inFIG. 11 , a laser beam L becomes a line beam after passing through thehomogenizer 4. That is, a cross section of the laser beam L orthogonal to an optical axis C is an elongated linear shape extending in one direction. For example, a cross section of the laser beam L orthogonal to the optical axis reflected by thereflection mirror 6 is a linear shape extending in the Y-axis direction. In order to crystallize the entire surface of the amorphous silicon film over the semiconductor film M, the semiconductor film M is moved along the short axis direction (X-axis direction) of the line beam intermittently at a feed pitch of 5 to 10% of the short axis width of the line beam in one shot of the line beam. For example, when the short axis width is 0.4 mm, the feed pitch is 20 to 40 and the number of times of the amorphous silicon film is irradiated with laser beams per location is 10 to 20 times. - When the solid-
state laser 2 emits a laser beam once, the semiconductor film M is irradiated with a laser beam twice at different timings. For example, when the solid-state laser 2 emits a laser beam seven times, the semiconductor film M is irradiated with the laser beams 14 times at different timings. The semiconductor film M is irradiated with the laser beams that have passed through the optical paths having different lengths, in accordance with the order of the respective lengths of the optical paths. That is, the semiconductor film M is irradiated firstly with the laser beam (corresponding to the above-described laser beam L1) through the first optical path PT1 having an optical path length shorter than that of the second optical path PT2. Then, the semiconductor film M is secondly irradiated with the laser beam (corresponding to the above-described laser beam L2) through the second optical path PT2. - Here, when a laser beam having energy density E0 is emitted once from the solid-
state laser 2, the energy density of the laser beam (corresponding to the above-described laser beam L1) that reaches the semiconductor film M first is defined as E1, and the energy density of the laser beam (corresponding to the above-mentioned laser beam L2) that reaches the semiconductor film M second is defined as E2. The reflectance of the firstpartial reflection mirror 3 a is defined as R1, the transmittance of the firstpartial reflection mirror 3 a is defined as T1, and the reflectance of the secondpartial reflection mirror 3 b is defined as R2. Then, E1 and E2 are respectively expressed by the following formulas. -
E1=T1·E0 -
E2=(R1·R2)·(E0) - From the above formulas, a ratio r of the energy density E2 of the laser beam (corresponding to the above-described laser beam L2) that reaches the semiconductor film M second to the energy density E1 of the laser beam (corresponding to the above-described laser beam L1) of the laser beam that reaches the semiconductor film M first is r=E2/E1=R1·R2/T1. Thus, the ratio r can be changed by appropriately changing R1, R2, and T1.
- In the method for manufacturing the semiconductor film M in the
laser processing apparatus 1 according to the second embodiment, first, the amorphous semiconductor film M is irradiated with the pulsed laser beam L1 through the first optical path PT1. After that, the semiconductor film M is irradiated with the laser beam L2 through the second optical path PT2 having intensity lower than that of the laser beam L1. By doing so, a waveform similar to the pulse waveform (FIG. 1 ) of the laser beam unique to the excimer laser is reproduced. Thus, the semiconductor film M having uniform crystal grain size and high crystalline quality can be formed. Further, since a solid-state laser is used in the method for manufacturing the semiconductor film M in thelaser processing apparatus 1 according to the second embodiment, maintainability is improved, and running cost can be reduced. Note that a flow of the method for manufacturing the semiconductor film M in thelaser processing apparatus 1 is the same as the above-described method for manufacturing the semiconductor film M according to the first embodiment (seeFIG. 7 ), and thus s description thereof will be omitted. - Next, as a third embodiment, a
laser processing apparatus 101 as another laser processing apparatus used in the above-described method for manufacturing the semiconductor film M according to the first embodiment will be described. -
FIG. 12 shows a configuration example of thelaser processing apparatus 101 according to the third embodiment. As shown inFIG. 12 , thelaser processing apparatus 101 further includes anattenuator 7 for attenuating a laser beam and adjusting the energy to predetermined energy density in addition to the components of the above-describedlaser processing apparatus 1 according to the second embodiment. That is, anoptical system module 110 includes theattenuator 7 as an optical element in addition to thepartial reflection mirror 3, thereflection mirror 6, and thehomogenizer 4. Theattenuator 7 is provided over the optical path between the solid-state laser 2 and the semiconductor film M. That is, theattenuator 7 is disposed over each optical path (first optical path PT1 and second optical path PT2) leading from the firstpartial reflection mirror 3 a and the secondpartial reflection mirror 3 b to thehomogenizer 4. Theattenuator 7 together with thepartial reflection mirror 3 has a role of adjusting the intensity of the laser beam applied to the semiconductor film M. That is, theattenuator 7 and thepartial reflection mirror 3 adjust the timing at which the semiconductor film M is irradiated with a laser beam next and adjust the intensity of this laser beam. - Like the above-described
laser processing apparatus 1 according to the second embodiment, in thelaser processing apparatus 101 according to the third embodiment, when a laser beam is emitted once from the solid-state laser 2, the semiconductor film M is irradiated with laser beams twice at different timings. For example, when the solid-state laser 2 emits a laser beam seven times, the semiconductor film M is irradiated with the laser beams 14 times at different timings. As described above, the semiconductor film M is firstly irradiated with the laser beam (corresponding to the above-described laser beam L1) through the first optical path PT1 having an optical path length longer than that of the second optical path PT2, and then secondly irradiated with the laser beam (corresponding to the above-described laser beam L2) through the second optical path PT2. - Here, when a laser beam having energy density E0 is emitted once from the solid-
state laser 2, the energy density of the laser beam (corresponding to the above-described laser beam L1) that reaches the semiconductor film M first is defined as E1, and the energy density of the laser beam (corresponding to the above-mentioned laser beam L2) that reaches the semiconductor film M second is defined as E2. The reflectance of the firstpartial reflection mirror 3 a is defined as R1, the transmittance of the firstpartial reflection mirror 3 a is defined as T1, and the reflectance of the secondpartial reflection mirror 3 b is defined as R2. An attenuation factor of anattenuator 7 a is defined as Ta0, an attenuation factor of anattenuator 7 b is defined as Ta1, and an attenuation factor of anattenuator 7 c is defined as Ta2. Then, E1 and E2 are respectively expressed by the following formulas. -
E1=(T1)·Ta1·(E0)·Ta0 -
E2=(R1·R2)·Ta2·(E0)·Ta0 - From the above formulas, a ratio r of the energy density E2 of the laser beam (corresponding to the above-described laser beam L2) that reaches the semiconductor film M second to the energy density E1 of the laser beam (corresponding to the above-described laser beam L1) of the laser beam that reaches the semiconductor film M first is r=E2/E1=(R1·R2/T1)·(Ta2/Ta1). Thus, the ratio r can be changed by appropriately changing R1, R2, T1, Ta1, and Ta2.
- In the above-described
laser processing apparatus 1 according to the second embodiment, the intensity of the laser beam is adjusted only by changing the transmittance of thepartial reflection mirror 3. On the other hand, in thelaser processing apparatus 101 according to the third embodiment, the intensity of the laser beam is finely adjusted by theattenuators 7 disposed over the first optical path PT1 and the second optical path PT2 in addition to changing the transmittance of thepartial reflection mirror 3. By doing so, it is possible to adjust the intensity of a laser beam more accurately. - Note that the method for manufacturing the semiconductor film M in the
laser processing apparatus 101 according to the third embodiment is the same as the above-described method for manufacturing the semiconductor film M in thelaser processing apparatus 1 according to the second embodiment, and thus a description thereof is omitted. - Next, as a fourth embodiment, a
laser processing apparatus 201 as another laser processing apparatus used in the method for manufacturing the semiconductor film M according to the first embodiment will be described. -
FIG. 13 shows a configuration example of thelaser processing apparatus 201 according to the fourth embodiment. In the above-describedlaser processing apparatus 1 according to the second embodiment, there is a single solid-state laser 2, whereas as shown inFIG. 13 , thelaser processing apparatus 201 according to the fourth embodiment includes a plurality of solid-state lasers 2 (solid-state lasers laser processing apparatus 201 according to the fourth embodiment further includes apulse generator 8 for applying laser beams from the plurality of solid-state lasers pulse generator 8 has a role of adjusting the timing of irradiating the semiconductor film M with laser beams. - In the
laser processing apparatus 201 according to the fourth embodiment, the laser beam emission timing of each of the solid-state lasers pulse generator 8 to thereby adjust an irradiation interval between a time when a laser beam is applied and a time when a laser beam is applied next. Further, thelaser processing apparatus 201 according to the fourth embodiment further includes, in anoptical system module 210,attenuators 7 for attenuating a laser beam and adjusting the energy to predetermined energy density in addition to optical elements such as thereflection mirror 6 and thehomogenizer 4. Theattenuators 7 are provided in respective optical paths (first optical path PT1 and second optical path PT2) from the solid-state lasers attenuator 7 has a role of adjusting the intensity of the laser beam applied to the semiconductor film M. That is, theattenuator 7 and thepulse generator 8 adjust the timing at which the semiconductor film M is irradiated with a laser beam next and adjust the intensity of this laser beam. Note that the intensity of the laser beam applied to the semiconductor film M may be adjusted by making the intensity of the laser beams emitted from the solid-state lasers - In the
laser processing apparatus 201 according to the fourth embodiment, when each of the solid-state lasers state lasers laser processing apparatus 201 according to the fourth embodiment, thepulse generator 8 adjusts the laser irradiation in such a way that the semiconductor film M is firstly irradiated with the laser beam (corresponding to the above-described laser beam L1) through the first optical path PT1, and then the semiconductor film M is secondly irradiated with the laser beam (corresponding to the above-described laser beam L2) through the second optical path PT2. - Here, the energy density of the laser beams emitted from the solid-
state lasers attenuator 7 d is defined as Ta3, and an attenuation factor of theattenuator 7 e is defined as Ta4. Then, E1 and E2 are respectively expressed by the following formulas. -
E1=Ta3·E0 -
E2=Ta4·E0 - From the above formulas, a ratio r of the energy density E2 of the laser beam (corresponding to the above-described laser beam L2) that reaches the semiconductor film M second to the energy density E1 of the laser beam (corresponding to the above-described laser beam L1) of the laser beam that reaches the semiconductor film M first is r=E2/E1=Ta4/Ta3. Thus, the ratio r can be changed by appropriately changing Ta3 and Ta4. Here, the energy density of the laser beams emitted from the solid-
state lasers state lasers - When there is only one solid-
state laser 2, like in the above-describedlaser processing apparatus 1 according to the second embodiment, a laser beam emitted from the solid-state laser 2 needs to be divided by an optical system such as thepartial reflection mirror 3 so that the divided laser beams pass through plurality of optical paths having different lengths to be applied to the semiconductor film M. On the other hand, in thelaser processing apparatus 201 according to the fourth embodiment, the configuration of the optical system can be simpler, and thus the space required for disposing the optical system can be reduced, thereby reducing the apparatus size. - Note that the method for manufacturing the semiconductor film M in the
laser processing apparatus 201 according to the fourth embodiment is the same as the above-described method for manufacturing the semiconductor film M in thelaser processing apparatus 1 according to the second embodiment, and thus a description thereof is omitted. - Next, as a fifth embodiment, a
laser annealing apparatus 301 as another laser processing apparatus used in the method for manufacturing the semiconductor film M according to the first embodiment will be described. Thelaser annealing apparatus 301 according to the fifth embodiment performs processing for irradiating the semiconductor film M formed over the substrate with a laser beam to crystallize the semiconductor film M. -
FIG. 14 shows a configuration example of thelaser annealing apparatus 301 according to the fifth embodiment. As shown inFIG. 14 , thelaser annealing apparatus 301 includes a solid-state laser 2, an optical system module 20, a sealingunit 30, and aprocessing chamber 40. Theprocessing chamber 40 is provided, for example, over a horizontal base (not shown). The sealingunit 30 is provided above theprocessing chamber 40, and the optical system module 20 is provided above the sealingunit 30. The optical system module 20 is provided at a position where the optical system module 20 can receive a laser beam L emitted from the solid-state laser 2. - Here, XYZ orthogonal coordinate axes are introduced in order to describe the
laser annealing apparatus 301. The direction orthogonal to the upper surface of the horizontal base is defined as a Z-axis direction, an upper direction of the Z-axis direction is defined as a +Z-axis direction, and a lower direction of the Z-axis direction is defined as a −Z-axis direction. The direction connecting the solid-state laser 2 to the optical system module 20 is defined as an X-axis direction, a direction from the solid-state laser 2 toward the optical system module 20 is defined as a +X-axis direction, and a direction opposite to the +X-axis direction is defined as a −X-axis direction. A direction orthogonal to the X-axis direction and the Z-axis direction is defined as a Y-axis direction, one direction of the Y-axis direction is defined as a +Y-axis direction, and a direction opposite to the +Y-axis direction is defined as a −Y-axis direction. - As shown in
FIG. 14 , the solid-state laser 2 is a laser light source that emits the laser beam L. The solid-state laser 2 is, for example, a YAG laser or a YVO laser. The solid-state laser 2 emits the laser beam L toward the optical system module 20. The laser beam L travels, for example, in the +X-axis direction and enters the optical system module 20. - The optical system module 20 includes an optical system casing 21 that constitutes an outer shape, optical elements such as a
reflection mirror 6, and a sealingwindow 23. The optical system casing 21 is a box-shaped member made of a material such as aluminum. Each optical element of the optical system module 20 is held inside the optical system casing 21 by a holder or the like. With such optical elements, the optical system module 20 adjusts the irradiation direction, the light amount, and the like of the laser beam L emitted from the solid-state laser 2. - The configuration of the above-described
optical system module 10 of thelaser processing apparatus 1 according to the second embodiment is applied as a configuration of the optical system module 20. The configuration of the above-describedoptical system module 110 of thelaser processing apparatus 101 according to the third embodiment or the above-described configuration of thelaser processing apparatus 201 of theoptical system module 210 according to the fourth embodiment may be applied as the configuration of the optical module 20. - The sealing
window 23 is provided over a part of the optical system casing 21, for example, over a lower surface of theoptical system casing 21. After the laser beam L is adjusted by the optical system module 20, the laser beam L is emitted from the sealingwindow 23 toward the sealingunit 30. In this way, the optical system module 20 irradiates the semiconductor film M with the laser beam L. -
FIG. 15 is a schematic diagram showing an example of a laser beam applied to the semiconductor film M. As shown inFIG. 15 , the laser beam L has a line beam shape in the optical system module 20. That is, the cross section of the laser beam L orthogonal to an optical axis C is an elongated linear shape extending in one direction. For example, a cross section of the laser beam L orthogonal to the optical axis of the laser beam L reflected by thereflection mirror 6 is a linear shape extending in the Y-axis direction. - As shown in
FIG. 14 , the sealingunit 30 includes a sealingcasing 31, a reflectedlight receiving member 61, a sealingwindow 33, agas inlet 34, and agas outlet 35. - The sealing
casing 31 is a box-shaped member with a hollow inside. Each of thegas inlet 34 and thegas outlet 35 is provided over a predetermined side surface of the sealingcasing 31. Thegas inlet 34 and thegas outlet 35 are provided, for example, over side surfaces of the sealingcasing 31 opposite to each other. For example, thegas outlet 35 is provided above thegas inlet 34. Agas 37, for example, an inert gas such as nitrogen is introduced from thegas inlet 34. Thegas 37 introduced inside the sealingcasing 31 from thegas inlet 34 is discharged from thegas outlet 35. It is desirable that thegas 37 be continuously supplied inside the sealingcasing 31. Further, it is desirable that thegas 37 be continuously discharged to the outside of the sealingcasing 31. A flow rate of thegas 37 is controlled to a predetermined flow rate so that the inside of the sealingcasing 31 is constantly ventilated. - The reflected
light receiving member 61 is disposed inside the sealingcasing 31. For example, the reflectedlight receiving member 61 is disposed outside the optical system module 20 in such a way that the reflectedlight receiving member 61 is spaced from the optical system module 20. The reflectedlight receiving member 61 is, for example, a plate-shaped member. The reflectedlight receiving member 61 is disposed with a plate surface facing the Z-axis direction. The reflectedlight receiving member 61 is disposed in such a way that it can receive a reflected beam R of the laser beam L reflected to the semiconductor film M. For example, the reflectedlight receiving member 61 is disposed over the optical path of the reflected beam R in consideration of an incident angle of the laser beam L and a reflection angle of the reflected beam R. Note that the reflectedlight receiving member 61 may be attached to the optical system module 20 with aheat insulating material 62 and a space therebetween. By doing so, heat insulation between the reflectedlight receiving member 61 and the optical system module 20 can be maintained. - The sealing
window 33 is provided over a part of the sealingcasing 31, for example, over a lower surface of the sealingcasing 31. The laser beam L emitted from the sealingwindow 23 of the optical system module 20 is emitted from the sealingwindow 33 of the sealingunit 30 toward theprocessing chamber 40. - The
processing chamber 40 includes agas box 41, asubstrate stage 45, asubstrate base 46, and ascanning apparatus 47. The semiconductor film M is disposed over thesubstrate stage 45 in a state in which the semiconductor film M is formed over a substrate (not shown). For example, in theprocessing chamber 40, the semiconductor film M disposed over thesubstrate stage 45 is irradiated with the laser beam L and then subject to laser annealing processing for crystallizing the semiconductor film M. Thesubstrate stage 45 may be a float type stage, i.e., a stage that transports the substrate over which the semiconductor film M is formed while the substrate is floated. - The
gas box 41 is a box-shaped member with a hollow inside. Thegas box 41 is disposed above thesubstrate stage 45 and below the sealingwindow 33 in the sealingunit 30. Anintroduction window 42 is provided over an upper surface of thegas box 41. Theintroduction window 42 is disposed to face the sealingwindow 33. Anirradiation window 43 is provided over a lower surface of thegas box 41. Theirradiation window 43 is disposed to face the semiconductor film M. - A
gas inlet 44 is provided over a predetermined side surface of thegas box 41. Apredetermined gas 37, for example, an inert gas such as nitrogen is supplied to thegas box 41 from thegas inlet 44. After the inside of thegas box 41 is filled with thegas 37 supplied to thegas box 41, thegas 37 is discharged from theirradiation window 43. - The laser beam L incident over the
gas box 41 is emitted from theirradiation window 43 and applied to the semiconductor film M. The reflectedlight receiving member 61 is disposed in such a way that it can receive the reflected beam R reflected by the semiconductor film M of the laser beam L applied to the semiconductor film M. - The
substrate stage 45 is disposed over thescanning apparatus 47 with, for example, asubstrate base 46 interposed therebetween. Thesubstrate stage 45 can be moved by thescanning apparatus 47 in the X-axis direction, the Y-axis direction, and the Z-axis direction. When the laser annealing processing is performed, thesubstrate stage 45 is transported by the scanning of thescanning apparatus 47, for example, in atransport direction 48 in the −X-axis direction. - Note that the method for manufacturing the semiconductor film M in the
laser annealing apparatus 301 according to the fifth embodiment is the same as the above-described method for manufacturing the semiconductor film M in thelaser processing apparatus 1 according to the second embodiment, and thus a description thereof is omitted. - Next, as a sixth embodiment, a method for manufacturing a semiconductor apparatus in the above-described laser processing apparatus will be described. In the sixth embodiment, the above-described
laser annealing apparatus 301 according to the fifth embodiment is used as a laser processing apparatus. The method for manufacturing a semiconductor apparatus according to the sixth embodiment includes a step of preparing an object to be processed including a substrate and an amorphous semiconductor film formed over the substrate and a step of irradiating the semiconductor film with a laser beam and crystallizing the semiconductor film. As the object to be processed, a substrate over which an amorphous semiconductor film is formed, for example, a glass substrate over which amorphous silicon is formed, is used. In the step of crystallizing the amorphous semiconductor film, laser annealing processing using the above-describedlaser annealing apparatus 301 according to the fifth embodiment is performed. - The semiconductor apparatus includes a TFT (Thin Film Transistor). In this case, an amorphous silicon film is irradiated with a laser beam and then crystallized, so that a polysilicon film is formed.
-
FIGS. 16 to 20 are cross-sectional views showing an example of the method for manufacturing a semiconductor apparatus according to the sixth embodiment. The above-describedlaser annealing apparatus 301 according to the sixth embodiment is suitable for manufacturing a TFT array substrate. Hereinafter, a method for manufacturing a semiconductor apparatus including a TFT will be described. - First, as shown in
FIG. 16 , agate electrode 92 is formed over aglass substrate 91. For example, a metal thin film containing aluminum or the like can be used as thegate electrode 92. Next, as shown inFIG. 17 , agate insulating film 93 is formed over thegate electrode 92. Thegate insulating film 93 is formed to cover thegate electrode 92. After that, as shown inFIG. 18 , anamorphous silicon film 94 is formed over thegate insulating film 93. Theamorphous silicon film 94 is disposed to overlap thegate electrode 92 with thegate insulating film 93 interposed therebetween. As described above, first, a substrate over which an amorphous semiconductor film is formed is prepared (Step A). - The
gate insulating film 93 is a silicon nitride film (SiNx), a silicon oxide film (SiO2 film), or a laminated film of these, etc. Specifically, thegate insulating film 93 and theamorphous silicon film 94 are continuously formed by a CVD (Chemical Vapor Deposition) method. Theamorphous silicon film 94 becomes the semiconductor film M in the laser processing apparatus. - Then, as shown in
FIG. 19 , theamorphous silicon film 94 is irradiated with a laser beam to crystallize theamorphous silicon film 94 using the above-describedlaser annealing apparatus 301 according to the fifth embodiment, so that apolysilicon film 95 is formed. For example, a first position control signal for controlling a disposed position of the substrate over thesubstrate stage 45 is transmitted to a loading/unloading apparatus (not shown) that loads and unloads the substrate (Step B). Then, the substrate is disposed by the loading/unloading apparatus at a first position over thesubstrate stage 45 determined by the first position control signal (Step C). After that, the substrate is transported over the substrate stage 45 (Step D), and the substrate is irradiated with a laser beam to polycrystallize an amorphous semiconductor film (Step E). After the amorphous semiconductor film is polycrystallized, the substrate is unloaded by the loading/unloading apparatus (Step F). - When all the irradiation areas are not irradiated, a second position control signal is further transmitted to the loading/unloading apparatus (Step G), and the substrate is disposed by the loading/unloading apparatus to a second position different from the first position over the
substrate stage 45 determined by the second position control signal (Step H). Then, the substrate is transported to a laser beam irradiation position over the substrate stage 45 (Step I), and the substrate is irradiated with a laser beam (Step J). Then, thepolysilicon film 95 in which silicon is crystallized is formed over thegate insulating film 93. - At this time, in the above-described
laser annealing apparatus 301 according to the fifth embodiment, first, the pulsed laser beam L1 from the solid-state laser 2 is applied, and after that, the pulsed laser beam L2 having intensity lower than that of the laser beam L1 is applied from the solid-state laser 2. By doing so, a waveform similar to the pulse waveform (FIG. 1 ) of the laser beam unique to the excimer laser is reproduced. Thus, the semiconductor film M having uniform crystal grain size and high crystalline quality can be formed. Further, since a solid-state laser is used, maintainability is improved, and running cost can be reduced. - After all the irradiation areas are irradiated and the semiconductor film is polycrystallized, the substrate is unloaded by the loading/unloading apparatus (Step K).
- After that, as shown in
FIG. 20 , aninterlayer insulating film 96, asource electrode 97 a, and adrain electrode 97 b are formed over thepolysilicon film 95. Theinterlayer insulating film 96, thesource electrode 97 a, and thedrain electrode 97 b can be formed by using a common photolithography method or film forming method. - A semiconductor apparatus provided with a TFT including a polycrystalline semiconductor film can be manufactured using the method for manufacturing a semiconductor apparatus according to the sixth embodiment. Such a semiconductor apparatus may be used for a screen of a display such as a liquid crystal display. Note that the subsequent manufacturing steps differ depending on the device to be eventually manufactured, and thus the description of the subsequent manufacturing steps will be omitted.
- As described above, the disclosure achieved by the inventor has been specifically described based on the embodiments. However, the present disclosure is not limited to the embodiments, and various modifications can be made without departing from the scope of the disclosure, as a matter of course. Further, the configuration in each embodiment may be appropriately exchanged between the embodiments.
- The first to sixth embodiments can be combined as desirable by one of ordinary skill in the art.
- From the disclosure thus described, it will be obvious that the embodiments of the disclosure may be varied in many ways. Such variations are not to be regarded as a departure from the spirit and scope of the disclosure, and all such modifications as would be obvious to one skilled in the art are intended for inclusion within the scope of the following claims.
Claims (8)
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JP3105488B2 (en) * | 1992-10-21 | 2000-10-30 | 株式会社半導体エネルギー研究所 | Laser treatment method |
JP3289681B2 (en) * | 1998-07-01 | 2002-06-10 | 日本電気株式会社 | Method for forming semiconductor thin film, pulsed laser irradiation device, and semiconductor device |
JP3707287B2 (en) * | 1998-09-03 | 2005-10-19 | セイコーエプソン株式会社 | Manufacturing method of semiconductor device |
EP1329946A3 (en) * | 2001-12-11 | 2005-04-06 | Sel Semiconductor Energy Laboratory Co., Ltd. | Manufacturing method of semiconductor device including a laser crystallization step |
US7470602B2 (en) * | 2002-10-29 | 2008-12-30 | Sumitomo Heavy Industries, Ltd. | Crystalline film and its manufacture method using laser |
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